chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
I 1 311 voltage divider giving an approximate lo4 to 1 voltage division. The "Charge" branch consists of the corona reactor in series with some value of Capacitance such that a voltage division of lo4 or lo3 to 1 will be obtained across the divider. The outputs from the low voltage ends of these dividers are fed to the X and Y axes of the oscilloscope. A variable potentiometer across the lower end of the "Charge" divider provides phase shift control to bring the "Voltage" and "Charge" branch outputs into phase for a null reading on the scope. It should be noted that two signals, of equal amplitude, in phase, fed to the X and Y axes of a scope, give a 45-degree line on the scope. Any variation of relative amplitude shifts the angle of the line. The area of the parallelogram represents the total power dissipated in the cell when the parallelogram bridge circuit and the oscilloscope are calibrated in the following manner: The X-axis deflection is calibrated with a peak reading voltmeter /so that reactor voltage (peak-to-peak) is presented as volts per cm of scope deflection. / The Y-axis deflection is calibrated with the known value of capacitance in the grounded end of the "Charge" branch so that the charge flowing through the reactor is presented as coulombs per cm /' of scope deflect ion. / The X - Y product, then, is: - ) (vo:~s,)(cou:;bs 1 volts - coulombs, watt-seconds cm2 or cm2 / . Since this is the energy per cm2 in one cycle, the power per cm2 of parallelogram area is obtained by multiplying the energy per cycle 2 by the frequency in reciprocal seconds. The parallelogram area can be , determined by planimeter measurement of a Polaroid picture, or by 'J direct measurement. \ With a dual beam oscilloscope it is also possible to view the a"/ voltage and charge waveforms simultaneously. \
FUFARCI! INSTITUTE OF TFYDLC UNIVERSTTY b150 KNRY P.VE. V'TIJDFLPPJA, PA. INTRODIJCTICN uses, Dlasma penerators, in general, have been found suitable for a variety of Thev penerally Drovide an electric arc which is condensed or constricted into a smaller circular cross-section than would ordinarily exist in an onen arc-tyDe device. This constriction penerates a very hinh temperature (8,000-20,000°K) so that a sunerheated-Dlasna workinp fluid can he ejected throuph the nozzle and the comoosition of the Dlasma determine the use to which the plasma nenerator is put. Plasma Fenerators have been used for cuttinn, welding, metal spravine and chemical orocessinr. For chemical processinp, plasma penerators have provided the possibility of the production of new aaloys and compounds and the processing of less commonly used materials, as well as the preoaration of certain common chemicals. nLAS#A JET EQUTPMrNT Two types of plasma generators are possible: the nontransferred and the transferred arc. A nontransferred arc consists of a cathode and a hollow anode where the arc is struck between the electrodes and the flame emerges through the orifice in the anode, In the transferred arc, the cathode is placed some distance away from the anode and an arc is passed between the electrodes. The nontransferred arc is the nost popular in the'chemical studies made to date. A plasma jet used in chemical synthesis can have varied desips to meet 1 special requirements, such as oath at a particular point. the introduction of a reactant material into the flame Consumable cathodes have been used in experiments in which carbon was one of \ the reactants, Carbon, vaporized from a graphite cathode, was used in the synthesis of cyanogen and hydrogen cyanide. powdered carbon introduced in a gas stream or as a constituent of a Kas has also been used as the source of carbon in a plasma flame. Electrodes of 2%-thoriated tungsten are the most frequently used water-cooled nonconsumable electrodes, Hater-cooled copper anodes have been widely used in experhens work. Figure 1 shows a typical plasma jet assembly. A reactor chamber may be of my confipuration desired to accomodate different feedinp: and quenching devices. PLASMA tTET REACTIONS GAS-CAS PEACTIONS TO PRODUCE A CAS AND CAS DFCO?'POS7TION PEACTIONS TO PFODUCF A GAS A considerable amount of research has been done by a number of people in the area of Dlasma jet eas-pas reactions. pases that have been investipated. The followinp is the gas reaction producing I \ \ i x \' x \ I t \'
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- Page 263 and 264: L ! , c PRODUCTS FROM A 28 MC. DISC
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- Page 269 and 270: a
- Page 271 and 272: 271 tube serve? as the high voltare
- Page 273 and 274: 273 ion (1L.). Zxcitei-ion by colli
- Page 275 and 276: Apparatus and Procedure 275 EXPERIM
- Page 277 and 278: . 277 6. A freshly prepared sam le
- Page 279 and 280: observed. The polystyrene (10% solu
- Page 281 and 282: i i (12) c (11) (14) I 281 LITERATU
- Page 283 and 284: FLOW- METER I ADDITIVE SUPPLY * ,28
- Page 285 and 286: 285 TABLE 2 Effect of Haloqenated A
- Page 287 and 288: ANALYTICAL RESULTS Some evidence wa
- Page 289 and 290: DISCUSSION 289 The salient features
- Page 291 and 292: ? ~ MENBERSHIP IN THE DIVISION OF F
- Page 293 and 294: 292 flow of the reactant gas stream
- Page 295 and 296: 294 have suitable residence times i
- Page 297 and 298: 0 E < h( E l! d K c 0 .- Y 0 t u t
- Page 299 and 300: 298 yields of many chemical product
- Page 301 and 302: - ;i Y . 15. Pressure lOmm 5 > 10-
- Page 303 and 304: 302 the best and in many practical
- Page 305 and 306: GENERATION AND MEASUREMENT OF AUDIO
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- Page 309 and 310: Vaccum-Tube Amplifier The mobile co
- Page 311: 310 f = Power supply frequency in c
- Page 316 and 317: J # I / 4) I . . '8 r4 0 r( P
- Page 318 and 319: 317 i Cuencb svsten w.nnar;itus use
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- Page 338 and 339: p .I V I .= - - HCN/C(CALC. WITH C
- Page 340 and 341: 1 1 339 atmospheric ressure and ach
- Page 342 and 343: RESULTS 341 Composition Dependence
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- Page 348 and 349: i 4 2 HYDROCARBON-NITROGEN REACTION
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- Page 356 and 357: ,) 355 The ceaswed conversion cf ni
- Page 358 and 359: 1 6 357 Freezing. 3jpotnesise thzf
- Page 360 and 361: 359 \ Frozen Compositior: Calcillat
FUFARCI! INSTITUTE OF TFYDLC UNIVERSTTY<br />
b150 KNRY P.VE.<br />
V'TIJDFLPPJA, PA.<br />
INTRODIJCTICN<br />
uses,<br />
Dlasma penerators, in general, have been found suitable for a variety <strong>of</strong><br />
Thev penerally Drovide an electric arc which is condensed or constricted<br />
into a smaller circular cross-section than would ordinarily exist in an onen arc-tyDe<br />
device. This constriction penerates a very hinh temperature (8,000-20,000°K) so<br />
that a sunerheated-Dlasna workinp fluid can he ejected throuph the nozzle and the<br />
comoosition <strong>of</strong> the Dlasma determine the use to which the plasma nenerator is put.<br />
Plasma Fenerators have been used for cuttinn, welding, metal spravine and <strong>chemical</strong><br />
orocessinr. For <strong>chemical</strong> processinp, plasma penerators have provided the possibility<br />
<strong>of</strong> the production <strong>of</strong> new aaloys and compounds and the processing <strong>of</strong> less commonly<br />
used materials, as well as the preoaration <strong>of</strong> certain common <strong>chemical</strong>s.<br />
nLAS#A JET EQUTPMrNT<br />
Two types <strong>of</strong> plasma generators are possible: the nontransferred and the<br />
transferred arc. A nontransferred arc consists <strong>of</strong> a cathode and a hollow anode<br />
where the arc is struck between the electrodes and the flame emerges through the<br />
orifice in the anode, In the transferred arc, the cathode is placed some distance<br />
away from the anode and an arc is passed between the electrodes. The nontransferred<br />
arc is the nost popular in the'<strong>chemical</strong> studies made to date.<br />
A plasma jet used in <strong>chemical</strong> synthesis can have varied desips to meet 1<br />
special requirements, such as<br />
oath at a particular point.<br />
the introduction <strong>of</strong> a reactant material into the flame<br />
Consumable cathodes have been used in experiments in which carbon was one <strong>of</strong> \<br />
the reactants, Carbon, vaporized from a graphite cathode, was used in the synthesis<br />
<strong>of</strong> cyanogen and hydrogen cyanide. powdered carbon introduced in a gas stream or as a<br />
constituent <strong>of</strong> a Kas has also been used as the source <strong>of</strong> carbon in a plasma flame.<br />
Electrodes <strong>of</strong> 2%-thoriated tungsten are the most frequently used water-cooled<br />
nonconsumable electrodes, Hater-cooled copper anodes have been widely used in experhens<br />
work. Figure 1 shows a typical plasma jet assembly. A reactor chamber may be <strong>of</strong> my<br />
confipuration desired to accomodate different feedinp: and quenching devices.<br />
PLASMA tTET REACTIONS<br />
GAS-CAS PEACTIONS TO PRODUCE A CAS AND CAS<br />
DFCO?'POS7TION PEACTIONS TO PFODUCF A GAS<br />
A considerable amount <strong>of</strong> research has been done by a number <strong>of</strong> people in<br />
the area <strong>of</strong> Dlasma jet eas-pas reactions.<br />
pases that have been investipated.<br />
The followinp is the gas reaction producing<br />
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